EP3315639A1 - Substrat de gan autoporteur, cristal gan, procédé de production d'un monocristal de gan et procédé de fabrication de dispositif semi-conducteur - Google Patents

Substrat de gan autoporteur, cristal gan, procédé de production d'un monocristal de gan et procédé de fabrication de dispositif semi-conducteur Download PDF

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EP3315639A1
EP3315639A1 EP17194202.2A EP17194202A EP3315639A1 EP 3315639 A1 EP3315639 A1 EP 3315639A1 EP 17194202 A EP17194202 A EP 17194202A EP 3315639 A1 EP3315639 A1 EP 3315639A1
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gan
substrate
self
plane
crystal
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EP3315639B1 (fr
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Satoru Nagao
Yusuke Tsukada
Kazunori Kamada
Shuichi Kubo
Hirotaka Ikeda
Kenji Fujito
Hideo Fujisawa
Yutaka Mikawa
Tae MOCHIZUKI
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Mitsubishi Chemical Corp
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    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L29/00Semiconductor devices specially adapted for rectifying, amplifying, oscillating or switching and having potential barriers; Capacitors or resistors having potential barriers, e.g. a PN-junction depletion layer or carrier concentration layer; Details of semiconductor bodies or of electrodes thereof ; Multistep manufacturing processes therefor
    • H01L29/02Semiconductor bodies ; Multistep manufacturing processes therefor
    • H01L29/12Semiconductor bodies ; Multistep manufacturing processes therefor characterised by the materials of which they are formed
    • H01L29/20Semiconductor bodies ; Multistep manufacturing processes therefor characterised by the materials of which they are formed including, apart from doping materials or other impurities, only AIIIBV compounds
    • H01L29/2003Nitride compounds
    • CCHEMISTRY; METALLURGY
    • C30CRYSTAL GROWTH
    • C30BSINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
    • C30B25/00Single-crystal growth by chemical reaction of reactive gases, e.g. chemical vapour-deposition growth
    • C30B25/02Epitaxial-layer growth
    • C30B25/18Epitaxial-layer growth characterised by the substrate
    • C30B25/186Epitaxial-layer growth characterised by the substrate being specially pre-treated by, e.g. chemical or physical means
    • CCHEMISTRY; METALLURGY
    • C30CRYSTAL GROWTH
    • C30BSINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
    • C30B25/00Single-crystal growth by chemical reaction of reactive gases, e.g. chemical vapour-deposition growth
    • C30B25/02Epitaxial-layer growth
    • C30B25/18Epitaxial-layer growth characterised by the substrate
    • C30B25/20Epitaxial-layer growth characterised by the substrate the substrate being of the same materials as the epitaxial layer
    • CCHEMISTRY; METALLURGY
    • C30CRYSTAL GROWTH
    • C30BSINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
    • C30B29/00Single crystals or homogeneous polycrystalline material with defined structure characterised by the material or by their shape
    • C30B29/10Inorganic compounds or compositions
    • C30B29/40AIIIBV compounds wherein A is B, Al, Ga, In or Tl and B is N, P, As, Sb or Bi
    • C30B29/403AIII-nitrides
    • C30B29/406Gallium nitride
    • CCHEMISTRY; METALLURGY
    • C30CRYSTAL GROWTH
    • C30BSINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
    • C30B7/00Single-crystal growth from solutions using solvents which are liquid at normal temperature, e.g. aqueous solutions
    • C30B7/10Single-crystal growth from solutions using solvents which are liquid at normal temperature, e.g. aqueous solutions by application of pressure, e.g. hydrothermal processes
    • C30B7/105Single-crystal growth from solutions using solvents which are liquid at normal temperature, e.g. aqueous solutions by application of pressure, e.g. hydrothermal processes using ammonia as solvent, i.e. ammonothermal processes
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L21/00Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
    • H01L21/02Manufacture or treatment of semiconductor devices or of parts thereof
    • H01L21/02104Forming layers
    • H01L21/02365Forming inorganic semiconducting materials on a substrate
    • H01L21/02367Substrates
    • H01L21/0237Materials
    • H01L21/02387Group 13/15 materials
    • H01L21/02389Nitrides
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L21/00Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
    • H01L21/02Manufacture or treatment of semiconductor devices or of parts thereof
    • H01L21/02104Forming layers
    • H01L21/02365Forming inorganic semiconducting materials on a substrate
    • H01L21/02518Deposited layers
    • H01L21/02521Materials
    • H01L21/02538Group 13/15 materials
    • H01L21/0254Nitrides
    • CCHEMISTRY; METALLURGY
    • C30CRYSTAL GROWTH
    • C30BSINGLE-CRYSTAL GROWTH; UNIDIRECTIONAL SOLIDIFICATION OF EUTECTIC MATERIAL OR UNIDIRECTIONAL DEMIXING OF EUTECTOID MATERIAL; REFINING BY ZONE-MELTING OF MATERIAL; PRODUCTION OF A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; SINGLE CRYSTALS OR HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; AFTER-TREATMENT OF SINGLE CRYSTALS OR A HOMOGENEOUS POLYCRYSTALLINE MATERIAL WITH DEFINED STRUCTURE; APPARATUS THEREFOR
    • C30B23/00Single-crystal growth by condensing evaporated or sublimed materials
    • C30B23/02Epitaxial-layer growth
    • C30B23/025Epitaxial-layer growth characterised by the substrate

Definitions

  • the present invention mainly relates to a nonpolar or semipolar self-standing GaN (gallium nitride) substrate.
  • a bar-shaped nonpolar or semipolar GaN substrate can be obtained by growing a GaN crystal along a c-axis on a 2 inch-diameter C-plane GaN template using an HVPE (Hydride Vapor Phase Epitaxy) method and slicing the GaN crystal so that a nonpolar or semipolar face becomes a principal surface (Patent Document 1). Furthermore, a plate-like nonpolar or semipolar GaN substrate can be fabricated from a GaN crystal vapor phase grown using a plurality of the bar-shaped GaN substrate arranged side by side as a seed (Patent Documents 1 to 3).
  • a method of fabricating an M-plane GaN substrate by slicing a hexagonal prism shape GaN crystal grown by a flux method and a method of using the M-plane GaN substrate as a seed to grow a bulk GaN crystal by an HVPE method and fabricating an M-plane GaN substrate by slicing the bulk GaN crystal are proposed (Patent Document 4).
  • a GaN crystal can be grown at a rate 100 times faster than a flux method.
  • a self-standing GaN substrate obtained by separating a GaN crystal grown by an HVPE method on a C-plane sapphire substrate on which a "void buffer layer" is formed from the sapphire substrate has been reported to have an a-axis length (also referred to as an a-axis lattice constant, an a-plane spacing, and the like) and a c-axis length (also referred to as a c-axis lattice constant, a c-plane spacing, and the like) of 3.189 ⁇ and 5.185 ⁇ , respectively (Non-patent Document 1).
  • Non-patent Document 2 A nitride semiconductor is also referred to as a GaN-based semiconductor, a group III nitride-based compound semiconductor, a nitride-based group III-V compound semiconductor, and the like and, in addition to including GaN (gallium nitride), includes a compound in which a part of or all of Ga in GaN is replaced with another element belonging to the thirteenth group in the periodic table (B, Al, or In). Examples include AlN, InN, AlGaN, AlInN, GaInN, and AlGaInN.
  • a (10-10) substrate, a (20-21) substrate, a (20-2-1) substrate, a (30-31) substrate, and a (30-3-1) substrate are particularly useful.
  • the (10-10) substrate (M-plane substrate) is a nonpolar substrate, while the (20-21) substrate, the (20-2-1) substrate, the (30-31) substrate, and the (30-3-1) substrate are semipolar substrates.
  • a main object of the present invention is to provide a self-standing nonpolar or semipolar GaN substrate having improved size and crystal quality.
  • the following inventions related to a self-standing GaN substrate, a crystal, a manufacturing method of a GaN single crystal, a manufacturing method of a semiconductor device, and the like are provided.
  • the following inventions related to a self-standing GaN substrate, a crystal, a method of producing a self-standing GaN substrate, a manufacturing method of a GaN single crystal, a manufacturing method of a semiconductor device, and the like are provided.
  • the following inventions related to a self-standing GaN substrate, a manufacturing method of a GaN single crystal, a manufacturing method of a semiconductor device, and the like are provided.
  • the following inventions related to a self-standing GaN substrate, a manufacturing method of a GaN single crystal, a manufacturing method of a semiconductor device, and the like are provided.
  • the following inventions related to a GaN crystal and a manufacturing method of a self-standing GaN substrate are provided.
  • a nonpolar or semipolar GaN substrate with improved size and crystal quality is provided.
  • a GaN crystal has a wurtzite type crystal structure belonging to the hexagonal crystal system.
  • a crystal axis parallel to [0001] is called a c-axis
  • a crystal axis parallel to [10-10] is called an m-axis
  • a crystal axis parallel to [11-20] is called an a-axis.
  • a crystal plane perpendicular to the c-axis is called a C-plane
  • a crystal plane perpendicular to the m-axis is called an M-plane
  • a crystal plane perpendicular to the a-axis is called an A-plane.
  • references made to a crystal axis, a crystal plane, a crystal orientation, and the like are assumed to mean a crystal axis, a crystal plane, a crystal orientation, and the like of a GaN crystal.
  • the A-plane in this case is assumed to mean an A-plane perpendicular to the M-plane that is parallel to or closest to parallel to the principal surface.
  • a name or Miller indices of a crystal plane that is attached to a name of a GaN substrate is that of a low index plane that is parallel to or closest to parallel to a front surface of the substrate.
  • the front surface refers to a surface intended to be used for forming a semiconductor device or epitaxially growing a crystal among the two principal surfaces of the substrate.
  • the principal surface that is not the front surface is referred to as a back surface.
  • a GaN substrate in which a low index plane that is parallel to or closest to parallel to a front surface thereof is an M-plane or, in other words, (10-10) is referred to as an M-plane substrate or a (10-10) substrate.
  • a crystal plane for which absolute values of integers h, k, m, and 1 of Miller indices (hkml) are equal to or smaller than 3 is assumed to be a low index plane.
  • a self-standing GaN substrate refers to a single crystal substrate consisting only of GaN crystal.
  • a self-standing GaN substrate may also be simply referred to as a GaN substrate.
  • a self-standing GaN substrate according to the present invention need only be thick enough to allow handling as a self-standing substrate.
  • the thickness varies depending on the size of the principal surface, the thickness can be empirically determined. In the case of a 2 inch-diameter disk-shaped substrate, a minimum thickness that enables the substrate to be handled as a self-standing substrate is normally 150 to 200 ⁇ m, a favorable thickness is 250 ⁇ m or more, and a further favorable thickness is 280 ⁇ m or more.
  • the thickness of a self-standing GaN substrate according to the present invention does not particularly have an upper limit, normally, the thickness is 1.5 mm or less. In the case of a 2 inch-diameter disk-shaped substrate, a thickness thereof is normally 400 ⁇ m or less and favorably 350 ⁇ m or less. However, depending on use a thicker substrate may be more favorable.
  • an angle between the normal of at least one principal surface and an m-axis is 0 degrees or more and 20 degrees or less.
  • at least one principal surface of a GaN substrate according to the present invention is parallel to a crystal plane whose angle of inclination from an M-plane is 0 degrees or more and 20 degrees or less.
  • [10-10], [20-21], [20-2-1], [30-31], and [30-3-1] form an angle with an m-axis that is 0 degrees or more and 20 degrees or less. Therefore, a (10-10) substrate, a (20-21) substrate, a (20-2-1) substrate, a (30-31) substrate, and a (30-3-1) substrate are included in a GaN substrate in which an angle between the normal of the principal surface and an m-axis is 0 degrees or more and 20 degrees or less.
  • an angle between the normal and an m-axis is 0 degrees or more and 20 degrees or less at each principal surface.
  • the size of the projected image in a c-axis direction when the principal surface is vertically projected on a M-plane is 10 mm or more.
  • the size in a c-axis direction is favorably 15 mm or more, more favorably 20 mm or more, more favorably 25 mm or more, more favorably 30 mm or more, more favorably 35 mm or more, more favorably 40 mm or more, more favorably 45 mm or more, and more favorably 50 mm or more.
  • the size of the projected image in an a-axis direction is normally 10 mm or more, favorably 20 mm or more, more favorably 30 mm or more, more favorably 40 mm or more, and more favorably 50 mm or more.
  • Fig. 1 shows a GaN crystal whose sizes in an a-axis direction, an c-axis direction, and an m-axis direction are respectively 20 mm, 10 mm, and 3.4 mm.
  • a substrate can be obtained in which an angle of inclination of the principal surface with respect to an M-plane is 10 degrees or less in an a-axis direction and within ⁇ 20 degrees in a c-axis direction and in which the size of the projected image when the principal surface is vertically projected on the M-plane is 20 mm in an a-axis direction and 10 mm in a c-axis direction.
  • the smaller the inclination angle of the principal surface with respect to the M-plane a larger number of the substrates can be cut out.
  • the a-axis length variation in the low distortion section is favorably 10.0 ⁇ 10 -5 ⁇ or less, more favorably 8.0 ⁇ 10 -5 ⁇ or less, and most favorably 6.0 ⁇ 10 -5 ⁇ or less.
  • a section length of the low distortion section is favorably 6 mm or more, more favorably 8 mm or more, and most favorably 10 mm or more.
  • the a-axis length can be measured using a reflection mode X-ray diffractometer. Measurement intervals are favorably 250 ⁇ m or less. An a-axis length is calculated based on a (300) lattice spacing obtaining by performing a 2 ⁇ - ⁇ scan of a (300) plane at each measurement point.
  • Fig. 2 shows a result of measurements of an a-axis length on a principal surface of a 50 mm (a-axis direction) ⁇ 25 mm (c-axis direction) ⁇ 346 ⁇ m (m-axis direction) self-standing M-plane GaN substrate according to the first embodiment as taken every 250 ⁇ m on a straight line parallel to a c-axis.
  • an intersection line between the principal surface and an A-plane is parallel to a c-axis.
  • a-axis length at each measurement point is plotted on a coordinate plane in which a horizontal axis thereof represents a position in a c-axis direction and a vertical axis thereof represents an a-axis length.
  • the graph shown in Fig. 2 has three low distortion sections, namely, a section A, a section B, and a section C.
  • the section A has an a-axis length variation width of 3.8 ⁇ 10 -5 ⁇
  • the section B has an a-axis length variation width of 3.5 ⁇ 10 -5 ⁇
  • the section C has an a-axis length variation width of 3.8 ⁇ 10 -5 ⁇ .
  • the section A has a section length of approximately 7 mm and the sections B and C respectively have section lengths of approximately 8 mm.
  • the GaN substrate When a low distortion section is observed in a measurement of a-axis lengths on one straight line, the GaN substrate may be described as including a low distortion region extending also in a direction that intersects with the straight line.
  • a GaN substrate according to the first embodiment Due to having a low distortion region, a GaN substrate according to the first embodiment has an advantage in that deformation occurring when the GaN substrate is heated inside a vapor phase growth furnace is small. Vapor phase epitaxial growth of a nitride semiconductor is normally performed while heating a substrate at a high temperature of 800°C or higher.
  • a variation in a c-axis length is favorably 3.0 ⁇ 10 -4 ⁇ or less and more favorably less than 2.0 ⁇ 10 -4 ⁇ .
  • an X-ray rocking curve full-width at half-maximum (XRC-FWHM) of a (300) plane is favorably less than 100 arcsec and more favorably less than 90 arcsec.
  • XRC-FWHM is smaller when dislocation density of a crystal is low.
  • a variation in the XRC-FWHM of a (300) plane is favorably less than 20 arcsec and more favorably less than 10 arcsec.
  • a longest one among the intersection lines may be selected and the measurement may be performed thereon.
  • a longest one among the intersection lines between a principal surface of a substrate and an A-plane means a longest intersection line formable by the principal surface and an A-plane.
  • a longest intersection line between the principal surface and an A-plane is a straight line (a dashed line in Fig. 3 ) parallel to a c-axis and passing through the center of the principal surface (center of a circle).
  • a portion at a distance of 2 mm or less from a substrate end surface may be excluded from consideration. This is because, in an outer peripheral portion of a substrate, defects attributable to mechanical processing of a crystal tend to remain and there are cases when a measurement value does not accurately reflect crystal quality.
  • a region excluding portions at a distance of 2 mm or less from a substrate end surface, of a principal surface of a substrate may be assumed to be an effective region, an a-axis length may be measured on a longest intersection line formable by the principal surface and an A-plane in the effective region, and crystal quality of the substrate may be evaluated based on a result of the measurement.
  • an a-axis length is within a range expressed as L a ⁇ 5.0 ⁇ 10 -5 ⁇ (where L a is a value equal to or larger than 3.1885 and smaller than 3.1895).
  • the a-axis length being within a range expressed as L a ⁇ 5.0 ⁇ 10 -5 ⁇ means that a variation width of the a-axis length on the longest intersection line is 10.0 ⁇ 10 -5 ⁇ or less.
  • L a ( ⁇ ) denotes a center value of the a-axis length on the longest intersection line and may be 3.1885 or larger and smaller than 3.1895.
  • the a-axis length on the longest intersection line is within a range expressed as L a ⁇ 4.0 ⁇ 10 -5 ⁇ and furthermore within a range expressed as L a ⁇ 3.0 ⁇ 10 -5 ⁇ .
  • a c-axis length is favorably within a range expressed as L c ⁇ 1.5 ⁇ 10 -4 ⁇ (where L c is a value equal to or larger than 5.1845 and smaller than 5.1865).
  • the c-axis length being within a range expressed as L c ⁇ 1 ⁇ 10 -4 ⁇ means that a variation width of the c-axis length on the longest intersection line is 3.0 ⁇ 10 -4 ⁇ or less.
  • L c ( ⁇ ) denotes a center value of the c-axis length on the longest intersection line and may be 5.1845 or larger and smaller than 5.1865.
  • the c-axis length on the longest intersection line is within a range expressed as L c ⁇ 1.0 ⁇ 10 -5 ⁇ .
  • an XRC-FWHM of a (300) plane is favorably less than 100 arcsec and more favorably less than 90 arcsec, and a variation width in the XRC-FWHM of a (300) plane is favorably less than 20 arcsec and more favorably less than 10 arcsec.
  • a self-standing GaN substrate according to the first embodiment may have an defect increasing zone extending in a direction intersecting an A-plane on the principal surface.
  • An defect increasing zone refers to a belt-like region in which density of crystal defects such as dislocations and stacking faults is locally high and is observed when a GaN crystal is grown by a method using an aggregated seed to be described later and a GaN substrate is fabricated from the GaN crystal. Specifically, in a GaN crystal grown on an aggregated seed, a portion with high defect density grown above a boundary between seed substrates constituting the aggregated seed appears as an defect increasing zone on a surface of a GaN substrate obtained by processing the GaN crystal.
  • dislocation density and stacking fault density measured in an arbitrarily-selected 300 ⁇ m x 400 ⁇ m area are respectively 1 ⁇ 10 4 to 1 ⁇ 10 6 cm -2 and 0 to 5 ⁇ 10 2 cm -1 outside the defect increasing zone
  • these defect densities inside the defect increasing zone are respectively 1 ⁇ 10 7 to 1 ⁇ 10 9 cm -2 and 1 ⁇ 10 3 to 1 ⁇ 10 5 cm -1 .
  • Fig. 4 is a perspective view of a disk-shaped M-plane GaN substrate having an defect increasing zone on a principal surface thereof.
  • the defect increasing zone extends along an a-axis direction.
  • a dotted line depicts an outer edge of the effective region of the substrate and a dashed line depicts a longest intersection line formable by a principal surface of the substrate and an A-plane in the effective region.
  • an a-axis length on a longest intersection line formable by the principal surface and a A-plane in the effective region is within a range expressed as favorably L a ⁇ 5.
  • L a may be a value equal to or larger than 3.1885 and smaller than 3.1895.
  • a length of this section is favorably less than 2 mm and more favorably less than 1.5 mm.
  • a c-axis length may also fall outside the preferred ranges described above, and, in addition, an XRC-FWHM of a (300) plane may also increase locally.
  • a self-standing GaN substrate according to the first embodiment is not limited by a manufacturing method of a GaN crystal used as a material, in a preferred example, the self-standing GaN substrate comprises a GaN crystal grown by an HVPE method.
  • a GaN crystal can be grown in which concentrations of undesirable impurities are kept lower than in a flux method or an ammonothermal method.
  • GaN crystal with a combined alkali metal concentration of lithium (Li), sodium (Na), and potassium (K) that is lower than 1 ⁇ 10 15 cm -3 Japanese Patent Application Laid-open No. 2009-18961 .
  • the same can be said of an ammonothermal method using an alkali metal as a mineralizer (Japanese Patent Application Laid-open No. 2011-523931 ).
  • a GaN crystal grown by an HVPE method normally has an alkali metal concentration of lower than 1 x 10 15 cm -3 .
  • a low concentration of alkali metals in a substrate is advantageous in terms of improving reliability of a semiconductor device to be formed on the substrate.
  • a GaN crystal can be obtained in which carrier concentration and conductivity are controlled with higher precision as compared with a flux method and an ammonothermal method.
  • a GaN crystal grown by an HVPE method has high transparency in a visible wavelength range and is suitable as a material of a GaN substrate for a light-emitting device.
  • a GaN crystal grown by an HVPE method has high transparency in a visible wavelength range and is suitable as a material of a GaN substrate for a light-emitting device.
  • an absorption coefficient of a GaN crystal grown by an ammonothermal method is 4 to 20 cm -1
  • an absorption coefficient of a GaN crystal grown by an HVPE method is 2 cm -1 or less ( T. Hashimoto, et al., Sensors and Materials, Vol. 25, No. 3 (2013) 155-164 ).
  • an HVPE method has an advantage of enabling a GaN crystal to grow at a significantly higher rate than a flux method and an ammonothermal method.
  • a self-standing GaN substrate according to the first embodiment may be manufactured according to, but not limited to, the following procedure.
  • the secondary GaN crystal is grown on a nitrogen polarity surface of the primary substrate.
  • a growth mask of a specific pattern (to be described later) is formed on the nitrogen polarity surface of the primary substrate.
  • an acidic mineralizer is used.
  • the secondary GaN crystal with small distortion in a crystal structure thereof can be grown at a high rate until a large size is attained.
  • an area of the secondary substrate can be increased and, consequently, an area of the tertiary substrate can be increased.
  • step (iii) is provided between steps (ii) and (iv).
  • Step (iii) is necessary because the secondary substrate fabricated in step (ii) cannot withstand temperature conditions that apply when growing a GaN crystal by an HVPE method. Due to a large number of voids contained in the secondary substrate, the secondary substrate breaks or deteriorates when subjected to high temperatures near 1000°C.
  • the secondary substrate can be used as a seed.
  • the tertiary substrate fabricated from the tertiary GaN crystal grown on the secondary substrate in step (iii) is similar to the secondary substrate in that distortion of a crystal structure thereof is small, and since the tertiary substrate is significantly superior to the secondary substrate with respect to heat resistance, the tertiary substrate can be favorably used as a seed when growing a GaN crystal by an HVPE method.
  • step (iv) There are two important points with respect to step (iv). Firstly, all of or approximately all of a carrier gas used when growing a GaN crystal by an HVPE method is constituted by nitrogen gas. Secondly, an upper surface of the seed is widened as much as possible.
  • the present inventors tried to use an aggregated seed in which a plurality of tertiary substrates are arranged so that respective end surfaces thereof come into close contact with each other and also tried to widen a principal surface of each tertiary substrate.
  • the primary GaN crystal to be used as a material of the primary substrate may be grown by any method.
  • a case where an HVPE method is used will now be described as an example.
  • a C-plane GaN template can be used as a seed.
  • a C-plane GaN template refers to a composite substrate which uses a single crystal substrate with a different chemical composition from GaN as a base member and which comprises a single crystal GaN layer grown thereon along c-axis by an MOCVD method or the like.
  • the surface of the single crystal GaN layer is a gallium polarity face.
  • the base member of the C-plane GaN template is a sapphire substrate, a GaAs substrate, a SiC substrate, a Si substrate, a Ga 2 O 3 substrate, an AlN substrate, or the like and a diameter thereof is normally 1 to 6 inches.
  • a thickness of the single crystal GaN layer is, for example, 0.5 to 50 ⁇ m.
  • a mask pattern for ELO may be provided on the surface of the single crystal GaN layer.
  • the mask pattern is formed by a thin film made of a material that inhibits vapor phase growth of GaN such as silicon nitride (SiN x ) and silicon oxide (SiO 2 ).
  • a preferred example of the mask pattern is a stripe pattern (line and space pattern). The direction of the stripes is set to be parallel to an m-axis of the single crystal GaN layer.
  • Growth of a GaN crystal by an HVPE method can be performed using a vapor phase growth apparatus of which a conceptual diagram is shown in Fig. 5 .
  • the vapor phase growth apparatus shown in Fig. 5 has a growth furnace 100, inlet pipes 101 to 103 for introducing gas into the growth furnace, a reservoir 104 that retains metallic gallium, a heater 105 arranged so as to enclose the growth furnace, a susceptor 106 for mounting a seed, and an exhaust pipe 107 for discharging gas from inside the growth furnace.
  • the growth furnace, the inlet pipes, the reservoir, and the exhaust pipe are formed of quartz.
  • the susceptor 106 is formed of carbon and, favorably the surface thereof is coated by SiC.
  • Ammonia (NH 3 ), gallium chloride (GaCl), and a carrier gas are supplied to the growth furnace 100 through the inlet pipes 101 to 103.
  • Gallium chloride is created by a reaction of hydrogen chloride (HCl) supplied to the reservoir 104 through the inlet pipe 102 with metallic gallium retained in the reservoir. Since the hydrogen chloride is supplied to the reservoir after being diluted by nitrogen gas (N 2 ), the gas introduced into the growth furnace through the reservoir contains hydrogen chloride and nitrogen gas in addition to gallium chloride.
  • HCl hydrogen chloride
  • N 2 nitrogen gas
  • Hydrogen gas (H 2 ) and nitrogen gas (N 2 ) are favorably used as the carrier gas.
  • a susceptor temperature during crystal growth may favorably be adjusted as appropriate within a range of 900 to 1200°C.
  • Internal pressure of the growth furnace during crystal growth may favorably be adjusted as appropriate within a range of 50 to 120 kPa.
  • the susceptor 106 is rotated so that a crystal grows uniformly on the seed.
  • the rotation rate may be adjusted as appropriate between, for example, 1 and 50 rpm.
  • the crystal growth rate is favorably set to a range of 80 to 300 ⁇ m/h.
  • the growth rate may be increased by increasing partial pressure of either one or both of GaCl and ammonia in the growth furnace.
  • the partial pressure of GaCl is favorably 2 ⁇ 10 2 to 2 ⁇ 10 3 Pa.
  • the partial pressure of ammonia is favorably 4 ⁇ 10 3 to 1 ⁇ 10 4 Pa.
  • Gas partial pressure as used herein means a value (P ⁇ r) obtained by multiplying pressure (P) in a growth furnace by a ratio (r) of a volumetric flow rate of specific gas among a sum of volumetric flow rates of all gases supplied into the growth furnace.
  • the primary substrate (C-plane GaN substrate) is fabricated by slicing, parallel to the C-plane, the primary GaN crystal grown on the C-plane GaN template. Details of techniques necessary for planarizing the principal surface and removing a damage layer are well known to those skilled in the art and need not be particularly described.
  • a nitrogen polarity surface of the primary substrate is subjected to a CMP (Chemical Mechanical Polishing) finish for planarization and removal of a damage layer.
  • the nitrogen polarity surface is a [000-1] side principal surface of a C-plane GaN substrate and is also called an N polarity face, a nitrogen face, and the like.
  • the secondary GaN crystal to be used as a material of the secondary substrate is grown by an ammonothermal method using the primary substrate as a seed.
  • a growth mask for limiting a region enabling crystal growth is formed on the nitrogen polarity surface of the primary substrate.
  • Fig. 6 is a schematic diagram exemplifying the primary substrate on which a growth mask is formed.
  • the primary substrate 1001 has a rectangular nitrogen polarity surface 1001a, and arranged thereon is a growth mask 1002 which has a linear opening with a width W o of around 50 to 100 ⁇ m and which has a stripe pattern (line and space pattern) parallel to an a-axis.
  • a stripe period P s is favorably set larger than 1 mm and is favorably set equal to or smaller than 10 mm.
  • An end surface 1001b in an a-axis direction and an end surface 1001c in a m-axis direction of the primary substrate must not be covered by the growth mask.
  • an outer peripheral portion of the nitrogen polarity surface may be exposed within a range of several mm from a substrate end surface.
  • the growth mask is formed by a metal that does not dissolve or decompose during growth of a GaN crystal by an ammonothermal method such as Al, W, Mo, Ti, Pt, Ir, Ag, Au, Ta, Ru, Nb, and Pd, or an alloy thereof.
  • an ammonothermal method such as Al, W, Mo, Ti, Pt, Ir, Ag, Au, Ta, Ru, Nb, and Pd, or an alloy thereof.
  • a raw material used in the ammonothermal method is favorably polycrystalline GaN.
  • Concentration of oxygen contained as an impurity in the polycrystalline GaN is favorably 5 ⁇ 10 19 cm -3 or lower.
  • An amount of impurities such as water and oxygen contained in ammonia used as a solvent is favorably 0.1 ppm or less.
  • An acidic mineralizer is used as a mineralizer.
  • a preferred example of the acidic mineralizer is an acidic mineralizer including a halogen element such as ammonium halide, gallium halide, and hydrogen halide. A combination of ammonium fluoride and hydrogen iodide is particularly favorable.
  • Growth of a GaN crystal by the ammonothermal method may be performed using a high-pressure growth apparatus of which a conceptual diagram is shown in Fig. 7 . Crystal growth is carried out in a cylindrical growth vessel 20 that is loaded into a cylindrical autoclave 1.
  • the growth vessel 20 is internally provided with a crystal growth zone 6 and a raw material dissolving zone 9 that are partitioned from each other by a baffle 5.
  • a seed crystal 7 suspended by a platinum wire 4 is installed in the crystal growth zone 6.
  • the raw material dissolving zone 9 is filled with raw material 8.
  • a gas line to which a vacuum pump 11, an ammonia cylinder 12, and a nitrogen cylinder 13 are connected is connected to the autoclave 1 via a valve 10.
  • a vacuum pump 11, an ammonia cylinder 12, and a nitrogen cylinder 13 are connected to the autoclave 1 via a valve 10.
  • an amount of ammonia supplied from the ammonia cylinder 12 can be checked using a mass flow meter 14.
  • the growth vessel 20 having a seed, the raw material, the mineralizer, and a solvent sealed therein is loaded into the autoclave 1, a space between the autoclave 1 and the growth vessel 20 is also filled with the solvent, and the autoclave 1 is hermetically sealed. Subsequently, the whole autoclave 1 is heated by a heater (not shown) to create a supercritical state or a subcritical state inside the growth vessel 20.
  • pressure inside the growth vessel 20 is favorably set to 180 MPa or higher and 300 MPa or lower and a temperature therein is favorably set to 530°C or higher and 650°C or lower.
  • the raw material dissolving zone 9 is kept at a higher temperature than the crystal growth zone 6. A difference in temperature between the two zones is favorably 80°C or less.
  • Fig. 8 schematically shows how the secondary GaN crystal grows.
  • the secondary GaN crystal 1003 is growing in a wall shape one by one above each opening of the growth mask 1002.
  • the height direction of the walls is a [000-1] direction (-c direction) and the thickness direction of the walls is an m-axis direction. While each of the walls also grows in the thickness direction, coalescence of adjacent walls is unlikely to occur.
  • a structure schematically shown in Fig. 9 is formed as a whole.
  • a GaN crystal that grows from an end portion 1001b in an a-axis direction of the primary substrate extends in the [000-1] direction and forms a wall 1004 having an inclined outer surface.
  • An end portion 1003b of the secondary GaN crystal in an a-axis direction connects to the inner surface of the wall 1004.
  • a GaN crystal that grows from an end portion 1001c in an m-axis direction of the primary substrate also extends in the [000-1] direction and forms a wall 1005 having an inclined outer surface.
  • the wall 1004 and the wall 1005 connect to each other to form a peripheral wall structure enclosing the secondary GaN crystal 1003.
  • the first effect is an effect of holding the secondary GaN crystal on the primary substrate.
  • the second effect is an effect of preventing the growth rate of the secondary GaN crystal in the [000-1] direction from slowing down.
  • the third effect is an effect of preventing the size of the secondary GaN crystal in an a-axis direction from decreasing.
  • the first effect enables regrowth in a growth process of the secondary GaN crystal.
  • Regrowth means an operation in which, at a time when a crystal is grown to a certain degree, the seed is taken out from the growth vessel and placed in a new growth vessel, and a crystal is once again grown on the seed. Since the growth rate declines as the raw material is consumed in the growth vessel, regrowth is essential to obtaining a large-size secondary GaN crystal. The formation of the structure shown in Fig. 9 enables such regrowth.
  • the structure is not formed, it is difficult to transfer the secondary GaN crystal from a used growth vessel to a new growth vessel while preventing the secondary GaN crystal from falling off from the primary substrate. This is because, as described previously, direct bonding between the secondary GaN crystal and the primary substrate is limited to inside of the long and narrow opening provided to the growth mask.
  • peripheral wall structure shown in Fig. 9 has an effect of protecting the secondary GaN crystal from suffering damage during handling.
  • a principal surface 2001a of the seed substrate is a nitrogen polarity surface and a shape thereof is a long and narrow rectangle extending in an a-axis direction.
  • a GaN crystal grows at a high rate on the nitrogen polarity surface of the seed substrate immediately after start of growth, but, at an early stage, stable faces 2002b and 2002c appear on a surface of a GaN crystal 2002 as shown in Fig. 10(b) . Since the stable faces 2002b and 2002c are both inclined with respect to the [000-1] direction that is a growth direction of the GaN crystal 2002, as crystal growth progresses, the nitrogen polarity surface 2002a of the GaN crystal narrows. Eventually, as shown in Fig. 10(c) , when an entire surface of the GaN crystal is occupied by the stable faces 2002b and 2002c and the nitrogen polarity surface 2002a disappears, the growth rate of the GaN crystal in the [000-1] direction drops to an impractical level.
  • the secondary GaN crystal can be grown in the [000-1] direction to 15 mm or more, 20 mm or more, or even 25 mm or more while maintaining the growth rate in the [000-1] direction to a practical level (for example, higher than 100 ⁇ m/day). Regrowth can be repeated twice or more.
  • the third effect described above can also be explained by a comparison with a model shown in Fig. 10 .
  • the model shown in Fig. 10 As the GaN crystal 2002 grows in the [000-1] direction, the size thereof in an a-axis direction decreases. This is because the stable face 2002b that appears at an end portion in an a-axis direction is inclined with respect to the c-axis.
  • the size of the secondary GaN crystal in an a-axis direction is generally determined in accordance with the size of the primary substrate in an a-axis direction.
  • the size of the primary substrate in an a-axis direction is dependent on the size of the C-plane GaN template that is used as a seed when growing the primary GaN crystal. Therefore, for example, by fabricating the primary substrate with a diameter exceeding 2 inches from the primary GaN crystal grown using a C-plane GaN template with a diameter of 3 inches and growing the secondary GaN crystal using the primary substrate as a seed, the secondary GaN crystal with a size in an a-axis direction of 2 inches (50 mm) or more can be obtained.
  • the size (thickness) of the secondary GaN crystal in an m-axis direction reaches approximately 1 mm or more (restricted by the stripe period P s of the growth mask 1002).
  • the secondary GaN crystal can be made into the secondary substrate (M-plane GaN substrate).
  • the secondary GaN crystal that is used as a material is desirably grown to 15 mm or more in a [000-1] direction.
  • the present inventors have confirmed that, by growing the secondary GaN crystal according to the method described above, the secondary substrate having a 52 mm ⁇ 52 mm rectangular principal surface can be fabricated.
  • the material of the secondary substrate is the secondary GaN crystal, the secondary substrate has low heat resistance and is not suitable as a substrate for epitaxially growing a nitride semiconductor by a vapor phase method such as a MOCVD method, an HVPE method, and the like.
  • the tertiary GaN crystal to be used as a material of the tertiary substrate is grown by an ammonothermal method using the secondary substrate as a seed.
  • Raw material, a solvent, and a mineralizer which may be favorably used when growing the tertiary GaN crystal are the same as those used when growing the secondary GaN crystal.
  • a usable crystal growth apparatus and favorable crystal growth conditions are also the same as those applicable to growing the secondary GaN crystal.
  • the portion of the GaN crystal which can be favorably used as a material for the tertiary substrate is an M-face grown portion formed on a principal surface of the secondary substrate.
  • an acidic mineralizer containing fluorine such as ammonium fluoride is particularly recommended when growing the tertiary GaN crystal.
  • This mineralizer has an effect of significantly accelerating the rate of M-face growth of a GaN crystal.
  • no basic mineralizers enabling M-face growth of a GaN crystal at a practical rate have been developed.
  • a GaN crystal ammonothermally grown using a fluorine-contained acidic mineralizer contains fluorine and concentration thereof normally exceeds 1 ⁇ 10 15 cm -3 .
  • the tertiary substrate (M-plane GaN substrate) is fabricated by slicing the tertiary GaN crystal parallel to an M-plane.
  • the principal surface is planarized by lapping and/or grinding and then subjected to a CMP finish to remove a damage layer.
  • the principal surface of the tertiary substrate is given a rectangular shape. Among four sides constituting the rectangle, two sides are arranged parallel to an a-axis and the other two sides are arranged parallel to a c-axis. Names of end surfaces of the tertiary substrate are defined as shown in Fig. 11 . Specifically, an end surface positioned at an end portion in an a-axis direction is called an A end surface. In addition, among end surfaces positioned at end portions in a c-axis direction, an end surface on a +c side ([0001] side) is called a +C end surface and an end surface on a -c side ([000-1] side) is called a -C end surface.
  • the +C end surface is a gallium polarity surface and the -C end surface is a nitrogen polarity surface.
  • Improving machining accuracy of the tertiary substrate and reducing variations of orientations of the principal surfaces and the end surfaces are extremely important for arranging a plurality of the tertiary substrates so that crystal orientations are aligned in the next step.
  • deviations from respective design values of an a-axis direction component and a c-axis direction component of an off-angle are made to be within ⁇ 0.2° and favorably within ⁇ 0.1°.
  • deviations from design values with respect to an a-axis direction and a m-axis direction are respectively made to be within ⁇ 0.2° and favorably within ⁇ 0.1°.
  • deviations from design values of the orientation of the A end surface with respect to a c-axis direction and an m-axis direction are respectively made to be within ⁇ 0.2° and favorably within ⁇ 0.1°.
  • the quaternary GaN crystal to be used as a material of the self-standing GaN substrate according to the first embodiment is grown by an HVPE method on an aggregated seed formed by arranging a plurality of tertiary substrates (M-plane GaN substrates).
  • Fig. 12(a) is a plan view of an aggregated seed formed by arranging five tertiary substrates side by side so that principal surfaces thereof face upward.
  • the tertiary substrates are arranged in an c-axis direction and, between adjacent tertiary substrates, the +C end surface of one tertiary substrate and the -C end surface of the other tertiary substrate are in contact with each other.
  • crystal orientations of the plurality of tertiary substrates constituting the aggregated seed can be precisely matched with one another.
  • an upper surface of the aggregated seed may be further expanded.
  • orientation accuracy of the A end surface of each tertiary substrate is also improved.
  • Fig. 12(b) is a sectional view showing a state where a GaN crystal grown by an HVPE method has covered the aggregated seed shown in Fig. 12(a) .
  • a GaN crystal that collectively covers five tertiary substrates can be grown.
  • Fig. 12(b) in a GaN crystal grown by an HVPE method, portions grown above boundaries between adjacent tertiary substrates are shown hatched. These portions tend to have a higher density of crystal defects such as dislocations and stacking faults than other portions.
  • a two-step growth method including (a) a temperature-raising step, (b) a preliminary growth step, and (c) a main growth step described below in this order is favorably performed.
  • a susceptor temperature is raised from room temperature to T 1 without supplying gallium chloride to the seed.
  • T 1 is favorably 830°C or higher and 870°C or lower.
  • a temperature raising rate is favorably 12°C/min or higher and 30°C/min or lower. The temperature raising rate may remain constant through the duration of the temperature-raising step or be changed during the temperature-raising step.
  • An atmospheric gas that may be introduced into the growth furnace in the temperature-raising step is hydrogen gas, ammonia, nitrogen gas, or the like.
  • At least both ammonia and nitrogen gas are introduced.
  • A. volumetric flow rate of ammonia introduced into the growth furnace is favorably 15% or more of a sum of volumetric flow rates of all gases introduced into the growth furnace.
  • the susceptor temperature is raised from T 1 to T 2 .
  • T 2 is favorably 940°C or higher and 1200°C or lower.
  • a temperature raising rate is favorably 6°C/min or higher and 24°C/min or lower.
  • GaCl partial pressure is favorably 2.0 ⁇ 10 2 Pa or higher and 5.0 ⁇ 10 2 Pa or lower and ammonia partial pressure is favorably 9.3 ⁇ 10 3 Pa or higher and 1.2 ⁇ 10 4 Pa or lower.
  • the carrier gas supplied into the growth furnace is to be constituted by nitrogen gas.
  • gallium chloride and ammonia are supplied onto the seed while maintaining the susceptor temperature at T 2 and a GaN crystal is grown until a thick film is formed.
  • the pressure in the growth furnace in the main growth step is favorably 50 kPa or higher and 120 kPa or lower.
  • GaCl partial pressure is favorably 1.5 ⁇ 10 2 Pa or higher and 5.0 ⁇ 10 2 Pa or lower and ammonia partial pressure is favorably 1.0 ⁇ 10 3 Pa or higher and 1.2 ⁇ 10 4 Pa or lower.
  • Fig. 13 shows an example of a profile of a susceptor temperature adoptable in the two-step growth method described above.
  • a temperature-holding step is provided between the temperature-raising step and the preliminary growth step.
  • a decomposition product of quartz constituting the growth furnace and the like is prevented from being adsorbed on a seed surface before the start of the main growth step.
  • the present inventors consider that a decomposition product of quartz is adsorbed on a seed surface to reduce its wettability with GaN and delay the occurrence of a step-flow growth mode of GaN.
  • GaN can be grown while supplying doping gas.
  • oxygen gas (O 2 ) or water (H 2 O) can be favorably used.
  • doping gas for silicon doping silane (SiH 4 ), disilane (Si 2 H 6 ), chlorosilane (SiH 3 Cl), dichlorosilane (SiH 2 Cl 2 ), trichlorosilane (SiHCl 3 ), tetrachlorosilane (SiCl 4 ), tetrafluorosilane (SiF 4 ), or the like can be favorably used.
  • oxygen doping of a GaN crystal can also be performed using oxygen-containing gas that is generated by decomposition of quartz constituting the growth furnace and the like. As the temperature of quartz members during crystal growth rises, an amount of generated oxygen-containing gas increases and oxygen concentration in the GaN crystal rises. When the oxygen concentration in the GaN crystal must be kept low, a method described in Japanese Patent Application Laid-open No. 2012-066983 can be applied. Examples are as follows.
  • a growth thickness of the quaternary GaN crystal is determined taking into consideration of a surface orientation of a self-standing GaN substrate to be fabricated. The thicker the quaternary GaN crystal, a GaN substrate with a larger angle between a principal surface thereof and an M-plane can be cut out.
  • the seed is separated from the quaternary GaN crystal by slicing or removed by grinding.
  • Types of processing performed when fabricating a self-standing GaN substrate from the quaternary GaN crystal are not limited. Necessary processing in accordance with required specifications of the substrate may be performed including core drilling, slicing, grinding, lapping, etching, CMP, and beveling.
  • At least one of the principal surfaces of the self-standing GaN substrate is planarized so that RMS roughness is reduced to less than 1 nm to ensure that the self-standing GaN substrate can be favorably used for epitaxial growth.
  • Planarization is favorably performed by, but not limited to, CMP.
  • a damage layer is favorably removed from the principal surfaces
  • a method of removal is not limited and may be arbitrarily selected from known methods including CMP, dry etching, and wet etching.
  • the self-standing GaN substrate according to the first embodiment can also be manufactured using the tertiary GaN crystal as referred to in the first method described above as a material.
  • Types of processing performed when fabricating the self-standing GaN substrate according to the first embodiment from the tertiary GaN crystal are not limited. Necessary processing in accordance with required specifications of the substrate may be performed including core drilling, slicing, grinding, lapping, etching, CMP, and beveling.
  • the self-standing GaN substrate manufactured by the second method has good heat resistance and may be preferably used as a substrate for epitaxially growing a nitride semiconductor by a vapor phase method such as an MOCVD method and an HVPE method.
  • the tertiary substrate is a M-plane GaN substrate.
  • an angle formed between a principal surface of the tertiary substrate and an m-axis is set to a relatively large angle.
  • a semipolar substrate such as a (30-31) substrate, a (30-3-1) substrate, a (20-21) substrate, and a (20-2-1) substrate is fabricated as the tertiary substrate.
  • a quaternary GaN crystal grows on the (30-31) substrate with a [30-31] direction as a thickness direction.
  • This quaternary GaN crystal may be processed to fabricate a self-standing GaN substrate according to the first embodiment. While it is obvious that a (30-31) substrate and a (30-3-1) substrate may be fabricated, substrates that can be fabricated are not limited thereto. By changing a slicing or polishing direction, a self-standing GaN substrate with various surface orientations such as a (20-21) substrate and an M-plane substrate can be fabricated from the quaternary GaN crystal.
  • a feature of a self-standing GaN substrate according to the second embodiment is that an anomalous transmission image can be obtained by transmission X-ray topography.
  • Fig. 14 is a diagram schematically showing an arrangement of an X-ray source, a test piece, and a detector in transmission X-ray topography by Lang's method.
  • An X-ray source is arranged on the side of one principal surface of a plate-like test piece with a thickness of t, and an X-ray detector is arranged on the side of the other principal surface.
  • An anomalous transmission of an X-ray is also called a Borrmann effect and is a phenomenon where an X-ray is transmitted through a crystal that is normally too thick for the x-ray to transmit due to absorption.
  • a transmission image is obtained from a GaN substrate with a thickness of 344 ⁇ m in X-ray topography using MoK ⁇ (wavelength 0.71073 ⁇ ) as an X-ray source, the image is an anomalous transmission image. This is because, an absorption coefficient ⁇ of GaN is 290.
  • ⁇ t 10.0 when the thickness t of a GaN substrate is 344 ⁇ m, and a transmission image cannot be obtained under a condition of ⁇ t ⁇ 10.0 unless an anomalous transmission occurs.
  • a GaN substrate according to the second embodiment may be the one for which an anomalous transmission is observed in a transmission X-ray topographic image acquired under a condition of ⁇ t ⁇ 10.0.
  • the size of the projected image when a principal surface thereof is vertically projected on an M-plane is a 10 mm square or more.
  • the size of the projected image in a c-axis direction is 15 mm or more and the size of the projected image in an a-axis direction is 25 mm or more.
  • the self-standing GaN substrate according to the second embodiment can be fabricated using the manufacturing method described previously in 2.1.2.
  • the self-standing GaN substrate according to the second embodiment may be a self-standing GaN substrate constituted by a GaN crystal grown by an HVPE method.
  • the self-standing GaN substrate according to the second embodiment can be fabricated from the tertiary GaN crystal as referred to in the manufacturing method of a self-standing GaN substrate described previously in 2.1.2.
  • a feature of a self-standing GaN substrate according to the third embodiment is that a dislocation density in an effective region of the principal surface is less than 4 ⁇ 10 5 cm -2 .
  • the dislocation density in an effective region of the principal surface as described herein means a dislocation density obtained by dividing a total number of dislocations existing in the effective region by an area of the effective region, the effective region being a region excluding portions at a distance of 2 mm or less from a substrate end surface, of the principal surface.
  • portions at a distance of 2 mm or less from a substrate end surface are removed is because an outer peripheral portion of a substrate is likely to retain defects attributable to mechanical processing of a crystal.
  • a region excluding an outer peripheral portion is used to form a semiconductor device. It is needless to say that, preferably, the outer peripheral portion also has a low defect density.
  • the dislocation density in the effective region of the principal surface is favorably less than 1 ⁇ 10 5 cm -2 and more favorably less than 4 ⁇ 10 4 cm -2 .
  • Dislocations on the principal surface of a GaN substrate can be observed as dark spots by a usual cathode luminescence (CL) method. Therefore, the dislocation density as used herein can be described as a density of dark spots observed by a CL method.
  • CL cathode luminescence
  • an etch pit with a size that is even detectable by an optical microscope can be formed at locations where dislocations exist.
  • Typical etching conditions include a sulfuric acid concentration of 85 to 90 wt%, a temperature of 265 to 275°C, and an etching time of 45 to 90 minutes.
  • the present inventors have confirmed that a density of etch pits formed by the heated sulfuric acid etching described above has a higher degree of coincidence with a dark spot density obtained by CL measurement as compared to other methods.
  • the number of dislocations existing on the principal surface of a substrate can also be obtained by counting the number of etch pits. In this case, using an optical microscope is convenient because a wide field of view can be observed.
  • the size of the projected image when the principal surface thereof is vertically projected on an M-plane is a 10 mm square or more.
  • the size of the projected image in a c-axis direction is 15 mm or more and the size of the projected image in an a-axis direction is 25 mm or more.
  • a material of the self-standing GaN substrate according to the third embodiment is, for example, the tertiary GaN crystal as referred to in the manufacturing method of a self-standing GaN substrate described previously in 2.1.2.
  • dislocation density of a self-standing GaN substrate obtained by processing the tertiary GaN crystal While there are variations in dislocation density of a self-standing GaN substrate obtained by processing the tertiary GaN crystal, even when such variations are taken into consideration, the dislocation density in the effective region of the principal surface rarely equals or exceeds 4 ⁇ 10 5 cm -2 . Although portions with high dislocation density and portions with low dislocation density are often formed on the principal surface with the substrate whose dislocation density is high, in such a case, an average dislocation density in a 200 ⁇ m ⁇ 200 ⁇ m region contained in the portion with high dislocation density is around 4 ⁇ 10 5 cm -2 at the maximum.
  • the substrate with a dislocation density in the effective region of the principal surface of 1 ⁇ 10 4 cm -2 has been produced. From what is known to date, for example, the smaller an off-angle of a principal surface of a seed used when growing the tertiary GaN crystal or, in other words, the higher the parallelism between the principal surface of the seed and an M-plane, the lower the dislocation density of the tertiary GaN crystal.
  • a portion near an outermost surface tends to have a higher dislocation density than a portion near a seed (the secondary substrate described previously). Therefore, in order to fabricate a self-standing substrate with a lower dislocation density, a portion relatively near the seed in the tertiary GaN crystal is desirably used as a material. However, there is a case where a portion adjacent to the seed has low heat resistance.
  • Types of processing performed when fabricating the self-standing GaN substrate according to the third embodiment from the tertiary GaN crystal are not limited. Necessary processing in accordance with required specifications of the substrate may be performed including core drilling, slicing, grinding, lapping, etching, CMP, and beveling.
  • a feature of a self-standing GaN substrate according to the fourth embodiment is that a stacking fault density in an effective region of the principal surface is less than 15 cm -1 .
  • the stacking fault density in an effective region of the principal surface as described herein means a stacking fault density obtained by dividing a total length of stacking faults existing in an effective region by an area of the effective region, the effective region being a region excluding portions at a distance of 2 mm or less from a substrate end surface, of the principal surface.
  • the stacking fault density in the effective region of the principal surface is favorably less than 5 cm -1 and more favorably less than 1 cm -1 .
  • a total length of stacking faults on a principal surface of a GaN substrate can be obtained by growing a GaN thin film by an MOCVD method on the principal surface and observing a surface of the thin film by an optical microscope.
  • the GaN thin film may be grown to a thickness of 2 ⁇ m using nitrogen gas as carrier gas and under conditions including an ammonia flow rate of 10 slm, a trimethyl gallium supply rate of 206 ⁇ mol/min, pressure of 12.5 kPa, and a substrate temperature of 1040°C.
  • a length of the stacking fault can be obtained by measuring a length of the step by optical microscope observation.
  • the size of the projected image when the principal surface thereof is vertically projected on an M-plane is a 10 mm square or more.
  • the size of the projected image in a c-axis direction is 15 mm or more and the size of the projected image in an a-axis direction is 25 mm or more.
  • a material of the self-standing GaN substrate according to the fourth embodiment is, for example, the tertiary GaN crystal as referred to in the manufacturing method of a self-standing GaN substrate described previously in 2.1.2.
  • the tertiary GaN crystal has a very low stacking fault density despite the parallelism between the growth direction and the c-axis being low.
  • a single tertiary GaN crystal has variations in crystallinity. For example, a portion near an outermost surface tends to have a higher stacking fault density than a portion near a seed (the secondary substrate described earlier). Therefore, in order to fabricate a self-standing substrate with fewer stacking faults, a portion relatively near the seed in the tertiary GaN crystal is desirably used as a material. However, there is a case where a portion adjacent to the seed has low heat resistance.
  • Types of processing performed when fabricating the self-standing GaN substrate according to the fourth embodiment from the tertiary GaN crystal are not limited. Necessary processing in accordance with required specifications of the substrate may be performed including core drilling, slicing, grinding, lapping, etching, CMP, and beveling.
  • the self-standing GaN substrate according to the present invention may be used as a seed for epitaxially growing a nitride semiconductor.
  • a GaN single crystal may be obtained by epitaxially growing GaN by an arbitrary method on the self-standing GaN substrate according to the present invention.
  • This GaN single crystal may be a bulk single crystal.
  • a first GaN single crystal may be fabricated by epitaxially growing GaN using the self-standing GaN substrate according to the present invention as a seed and, subsequently, a second GaN single crystal may be fabricated by epitaxially growing GaN using a part of or all of the first GaN single crystal as a seed.
  • This second GaN single crystal may be a bulk single crystal.
  • a GaN substrate including a seed portion can be fabricated.
  • the self-standing GaN substrate according to the present invention may also be used to manufacture a semiconductor device. Normally, one or more types of nitride semiconductors are epitaxially grown on the self-standing GaN substrate according to the present invention to form a device structure.
  • an epitaxial growth method an MOVCD method, an MBE method, a pulsed deposition method, or the like suitable for forming a thin film may be favorably used.
  • a semiconductor device examples include a light-emitting device such as a light-emitting diode and a laser diode, an electronic device such as a rectifier, a bipolar transistor, a field effect transistor, and an HEMT (High Electron Mobility Transistor), a semiconductor sensor such as a temperature sensor, a pressure sensor, a radiation sensor, and a visible-ultraviolet light detector, and the like.
  • a light-emitting device such as a light-emitting diode and a laser diode
  • an electronic device such as a rectifier, a bipolar transistor, a field effect transistor, and an HEMT (High Electron Mobility Transistor)
  • a semiconductor sensor such as a temperature sensor, a pressure sensor, a radiation sensor, and a visible-ultraviolet light detector, and the like.
  • the self-standing GaN substrate according to the present invention may also be applied to use including a SAW (Surface Acoustic Wave) device, a vibrator, a resonator, an oscillator, a MEMS (Micro Electro Mechanical System) component, a voltage actuator, and an electrode for an artificial photosynthesis device.
  • SAW Surface Acoustic Wave
  • MEMS Micro Electro Mechanical System
  • a GaN layer-bonded substrate may be manufactured using the self-standing GaN substrate according to the present invention as a material.
  • a GaN layer-bonded substrate refers to a composite substrate in which a GaN layer is bonded to a hetero-composition substrate with a different chemical composition from GaN and can be used to manufacture a light-emitting device and other semiconductor devices.
  • a GaN layer-bonded substrate is manufactured by executing, in this order, the steps of: implanting ions in a vicinity of a principal surface of a GaN substrate; bonding the principal surface side of the GaN substrate to a hetero-composition substrate; and forming a GaN layer bonded to the hetero-composition substrate by separating the GaN substrate at the ion-implanted region as a boundary.
  • a GaN layer-bonded substrate having a structure in which a GaN layer separated from the self-standing GaN substrate according to the present invention is bonded to a hetero-composition substrate.
  • an initial thickness of the self-standing GaN substrate according to the present invention may be 1 mm or more, 2 mm or more, or 4 mm or more.
  • hetero-composition substrates that may be used to manufacture a GaN layer-bonded substrate include a sapphire substrate, an AlN substrate, a SiC substrate, a ZnSe substrate, a Si substrate, a ZnO substrate, a ZnS substrate, a quartz substrate, a spinel substrate, a carbon substrate, a diamond substrate, a Ga 2 O 3 substrate, a ZrB 2 substrate, a Mo substrate, and a W substrate.
  • a GaN crystal (primary GaN crystal) was grown by an HVPE method on a sapphire-based C-plane GaN template with a striped mask pattern for ELO formed on a principal surface thereof.
  • a C-plane GaN substrate (primary substrate) with a rectangular principal surface having vertical and horizontal sides respectively parallel to an a-axis and an m-axis was fabricated from the GaN crystal.
  • a nitrogen polarity surface of the C-plane GaN substrate was made into a flat surface with no damage layer by performing a CMP finish.
  • a growth mask with a stripe pattern having 100 ⁇ m-wide linear openings at a period of 1100 ⁇ m was formed with a TiW alloy on the nitrogen polarity surface of the primary substrate fabricated in [1] above.
  • a longitudinal direction of the openings or, in other words, a stripe direction was arranged parallel to the a-axis.
  • a GaN crystal (secondary GaN crystal) was grown by an ammonothermal method using the primary substrate as a seed.
  • Polycrystalline GaN manufactured by a method of causing a vapor phase reaction of NH 3 and GaCl was used as a raw material and ammonium fluoride (NH 4 F) and hydrogen iodide (HI) were used as mineralizers.
  • Charge amounts of NH 4 F and HI were determined so that a molar ratio of fluorine atoms to NH 3 was 0.5 to 1.5%, a molar ratio of iodine atoms to NH 3 was 1.5 to 3.5% and, a molar ratio of fluorine atoms to iodine atoms was 0.2 to 0.5.
  • Growth conditions included setting an average temperature inside a growth vessel (an average value of temperatures in a crystal growth zone and a raw material dissolving zone) to 590 to 615°C, a difference in temperatures between the crystal growth zone and the raw material dissolving zone to 10 to 25°C, and pressure inside the growth vessel to 200 to 220 MPa.
  • a growth period was set to a total of 58 days or more excluding time required for replacing growth vessels for regrowth.
  • a structure shown in Fig. 9 was formed by the GaN crystal ammonothermally grown on the primary substrate. From a portion grown in a wall shape on each opening of the growth mask in the grown GaN crystal (secondary GaN crystal), an M-plane GaN substrate (secondary substrate) with a length of 50 to 54 mm, a width of 8 to 11 mm, and a thickness of 280 to 320 ⁇ m and having a rectangular principal surface with a long side parallel to an a-axis and a short side parallel to a c-axis was fabricated. Both principal surfaces of the secondary substrate were subjected to a CMP finish.
  • a GaN crystal (tertiary GaN crystal) was further grown by an ammonothermal method using the secondary substrate fabricated in [2] above as a seed.
  • the charge amount of the mineralizer were set such that molar ratios of fluorine atoms and iodine atoms to NH 3 were respectively 0.5% and 1.5%.
  • the average temperature inside the growth vessel was set to 600 to 611°C
  • the difference in temperatures between the crystal growth zone and the raw material dissolving zone was set to 9 to 13°C
  • the growth period was set to 15 days or more.
  • an M-plane GaN substrate (tertiary substrate) with a length of 41 to 59 mm, a width of 5 to 1.1 mm, and a thickness of 330 ⁇ m and having a rectangular principal surface with a long side parallel to an a-axis and a short side parallel to a c-axis was fabricated.
  • a side to be used for epitaxial growth of a quaternary GaN crystal in a next step was given an off-angle of -2° in a [0001] direction.
  • the accuracies of a [0001] direction component and a [11-20] direction component of the off-angle were respectively set to ⁇ 0.1°.
  • a +C end surface and a -C end surface were arranged parallel to a C-plane and respectively given inclinations within ⁇ 0.1° in a [10-10] direction and a [11-20] direction.
  • a end surfaces were arranged parallel to an A-plane and respectively given inclinations within ⁇ 0.1° in a [0001] direction and a [10-10] direction.
  • the principal surfaces of the tertiary substrate were finished by a CMP process.
  • a GaN crystal was grown by an HVPE method using an aggregated seed prepared by aligning seven tertiary substrates fabricated in [3] above side by side in a c-axis direction with their front surfaces facing upward.
  • the seven tertiary substrates were closely aligned so that, between two adjacent substrates, the +C end surface of one substrate came into contact with the -C end surface of the other substrate.
  • the two-step growth method described earlier was used. In other words, at first, while only supplying nitrogen gas and ammonia to the seed, a susceptor temperature was raised to 850°C (temperature-raising step) and the temperature was maintained for 5 seconds (temperature-holding step).
  • gallium chloride and ammonia were supplied onto the seed while keeping the temperature constant to grow GaN for 97 hours (main growth step).
  • pressure inside the growth furnace was controlled at 1.0 ⁇ 10 5 Pa
  • GaCl partial pressure was controlled at 2.1 ⁇ 10 2 Pa
  • ammonia partial pressure was controlled at 5.7 ⁇ 10 3 Pa.
  • Carrier gas supplied into the growth furnace was entirely constituted by nitrogen gas.
  • the grown GaN crystal collectively covered the seven tertiary substrates and the thickness thereof was 6. 8 mm at a central portion of the seed.
  • the thickness of the GaN crystal decreased from the central portion toward an outer peripheral portion of the aggregated seed and was 4. 5 mm at the portion near the +c side ([0001] side) end and 5.5 to 6.2 mm at the portion near the -c side ([000-1] side) end.
  • a self-standing M-plane GaN substrate with a length of 50 mm, a width of 25 mm, and a thickness of 346 ⁇ m and having a rectangular principal surface with a long side parallel to an a-axis and a short side parallel to a c-axis was cut out.
  • the principal surface on the X-ray incident side in the X-ray analysis performed later was given an off-angle of -2.0° ⁇ 0.1° in a [0001] direction and 0.0° ⁇ 0.1° in a [-12-10] direction.
  • the principal surface was first planarized by lapping and then subjected to a CMP finish for further planarization and removal of a damage layer.
  • the M-plane GaN substrate was fixed to a sample stage so that the c-axis direction was horizontal and the a-axis direction was vertical. Then, X-rays were made incident to the principal surface of the sample to perform a 2 ⁇ - ⁇ scan of a (300) plane and a (20-3) plane every 250 ⁇ m on a straight line parallel to a c-axis direction.
  • a Ge (220) 3-bounce monochromator (a so-called analyzer) and a proportional counter detector were used on a light-receiving side.
  • the temperature inside a housing of the X-ray diffractometer was controlled within 24.5 ⁇ 1°C. The origin of 20 was calibrated upon start of measurement and checked for deviations at the end of the measurement.
  • XRD analysis software [PANalytical X'Pert Epitaxy] manufactured by Spectris Co., Ltd. was used to fit a spectrum of the 2 ⁇ - ⁇ scan by a Gaussian function to obtain a peak, and the lattice spacing was derived by a calculation based on dynamical theory from the value of the peak.
  • Measurements of lattice spacing were performed with respect to the (300) plane and the (20-3) plane.
  • the (300) plane was selected because, compared to a (100) plane, 2 ⁇ is measured at a higher angle side and, consequently, a measurement with higher angular resolution can be performed.
  • An a-axis length was obtained from the (300) lattice spacing and a c-axis length was calculated based on the (300) lattice spacing and the (20-3) lattice spacing.
  • the c-axis length was obtained by expressions (2) and (3) below from the (300) lattice spacing and the (20-3) lattice spacing.
  • ⁇ 1 in expression (1) and ⁇ 2 in expression (3) are, respectively, correction coefficients for refraction correction of the values of the a-axis length and the c-axis length.
  • the correction coefficients were calculated by referring to " The Study of Imperfections in Semiconductor Single Crystals by Precise Measurements of Lattice Parameters" by Yasumasa Okada in “Researches of Electrotechnical Laboratory” Volume 913 (June 1990) (ISSN: 0366-9106 ) and using expression (4) below.
  • 4.48 ⁇ 10 ⁇ 7 ⁇ n 0 ⁇ 2 cos ⁇ sin ⁇ + ⁇ ⁇ sin ⁇ ⁇ ⁇
  • a variation width of the a-axis length was 4. 9 ⁇ 10 -5 A in all sections excluding two exceptional sections.
  • the exceptional sections were a section with a c-axis direction position of -6.5 mm to -6 mm and a section with a c-axis direction position of 2.25 mm to 3.5 mm.
  • the exceptional sections corresponded to portions constituted by GaN crystals having grown above boundaries between adjacent tertiary substrates and exhibited a large local variation in the a-axis length. Lengths of both exceptional sections were less than 1.5 mm.
  • a variation width of the c-axis length was 1.8 ⁇ 10 -4 A in all sections excluding end portions and two exceptional sections.
  • the exceptional sections were a section with a c-axis direction position of -6.5 mm to -6 mm and a section with a c-axis direction position of 2.25 mm to 3.5 mm.
  • the exceptional sections corresponded to portions constituted by GaN crystals having grown above boundaries between adjacent tertiary substrates and exhibited a large local variation in the c-axis length. Lengths of both exceptional sections were less than 2 mm.
  • a variation width of the a-axis length and a variation width of (300) lattice spacing will now be described. Since the relationship between the a-axis length (after refraction correction) and (300) lattice spacing (measured value) is as represented by expression (1) above, a variation in the a-axis length of 10.0 ⁇ 10 -5 A or less means that a variation width of (300) lattice spacing is less than 2.9 ⁇ 10 -5 ⁇ .
  • the XRC-FWHM was less than 85 arcsec excluding two exceptional sections.
  • the exceptional sections were a section with a c-axis direction position of -7.25 mm to -5.5 mm and a section with a c-axis direction position of 3.25 mm to 4 mm.
  • a variation in the XRC-FWHM increased and spots where the value of the XRC-FWHM was prominently high were observed.
  • These exceptional sections corresponded to portions constituted by GaN crystals having grown above boundaries between adjacent tertiary substrates.
  • a variation width of the XRC-FWHM was less than 10 arcsec excluding the two exceptional sections.
  • a long line-focus tube with a Cu target was used in a line focus mode, and an incident optical system including a divergence slit, a 50 ⁇ m mask, and a mirror for increasing beam parallelism was used.
  • an incident optical system including a divergence slit, a 50 ⁇ m mask, and a mirror for increasing beam parallelism was used.
  • a semiconductor two-dimensional detector with an element size of 55 ⁇ m ⁇ 55 ⁇ m and a detector size of 14 mm ⁇ 14 mm was used.
  • Fig. 18 shows a reflection X-ray topographic image obtained using (203) diffraction of a portion (a portion not including a crystal grown above a boundary between adjacent tertiary substrates) of the M-plane GaN substrate.
  • a striped pattern in a horizontal direction is seen in the image shown in Fig. 18 .
  • This striped pattern does not represent a distortion of the crystal. Instead, since there is periodicity in the a-axis direction, it is understood that the striped pattern represents an intensity variation of diffraction rays appeared due to an intensity variation in incident X-rays.
  • the density of the striped pattern is uniform or, in other words, the intensity variation of diffraction rays reflects only the intensity variation of the incident X-rays.
  • a crystal lattice structure of the GaN crystal constituting the substrate is uniform not only in a c-axis direction but also in an a-axis direction. Based on the X-ray topograph, it was presumed that the measurements of lattice spacing and rocking curves described above will produce approximately the same result even when carried out at different positions.
  • the present inventors measured an a-axis length on the principal surface on two parallel straight lines.
  • the two straight lines were respectively parallel to the c-axis and spacing (a distance in an a-axis direction) between the two straight lines was 5 mm.
  • the measurement was performed every 250 ⁇ m on each straight line.
  • a low distortion section with an a-axis length variation of less than 5 ⁇ 10 -5 ⁇ was observed over 10 to 11 mm on both straight lines.
  • An M-plane GaN substrate was fabricated by the same procedure as Experiment 1 above with the exception of changing the carrier gas used when growing a GaN crystal by an HVPE method on a seed constituted by tertiary substrates.
  • Fig. 21 shows a reflection X-ray topographic image obtained using (203) diffraction of a portion (a portion not including a crystal grown above a boundary between adjacent tertiary substrates) of a GaN substrate of a comparative example fabricated in Experiment 2.
  • the M-plane GaN substrate according to Experiment 2 has larger variations in the a-axis length and the c-axis length and greater disturbance of crystal as compared to the M-plane GaN substrate according to Experiment 1 described previously.
  • a reflection X-ray topographic image shown in Fig. 21 exhibits extremely sharp contrast between light and dark portions and has extremely low uniformity of diffraction intensity. This indicates that the crystal is significantly distorted.
  • a self-standing M-plane GaN substrate was fabricated in a similar manner to Experiment 1 described earlier. However, in Experiment 3-1, the size in a c-axis direction of the secondary GaN crystal fabricated by the first ammonothermal growth was enlarged and, accordingly, sizes of the secondary substrate and the tertiary substrate in a c-axis direction were enlarged.
  • the M-plane GaN substrate according to Experiment 3-1 has a large crystal disturbance at an end portion whose c-axis direction position exceeds 11 mm. Upon use, this portion is favorably removed.
  • variation widths of the a-axis length and the c-axis length were respectively 5.9 ⁇ 10 -5 A and 1.9 ⁇ 10 -4 ⁇ excluding two exceptional sections.
  • the exceptional sections were a section with a c-axis direction position of -6.75 mm to -5.75 mm and a section with a c-axis direction position of 5.5 mm to 6.25 mm. These sections corresponded to portions constituted by GaN crystals having grown above boundaries between adjacent tertiary substrates and exhibited large local variations in the a-axis length and the c-axis length. Lengths of both exceptional sections were less than 1.5 mm.
  • a self-standing M-plane GaN substrate was fabricated in a similar manner to Experiment 1 described previously.
  • An external view photograph of the self-standing GaN substrate is shown in Fig. 24(a) .
  • the substrate Although the substrate is shown to be cracked in the external view photograph, this was due to inappropriate handling.
  • the substrate had a thickness of 240 ⁇ m and did not crack when handled appropriately.
  • a transmission X-ray topographic image was acquired using one of the pieces of the self-standing M-plane GaN substrate shown in Fig. 24(a) as a sample.
  • the X-RAY Topographic Imaging System XRT-300 by Rigaku Corporation was used for X-ray topography.
  • MoK ⁇ was used as an X-ray source and an imaging plate with a pixel size of 50 ⁇ m was used as a detector.
  • a transmission X-ray topograph shown in Fig. 24 (b) was obtained using (002) diffraction.
  • a self-standing M-plane GaN substrate was fabricated in a similar manner to Experiment 1 above with the exception of changing the carrier gas used when growing a GaN crystal by an HVPE method on a seed constituted by the tertiary substrate.
  • Figs. 25 and 26 show that variations in the a-axis length and the c-axis length are relatively large on a straight line parallel to the c-axis on the principal surface of the M-plane GaN substrate of Experiment 4.
  • a self-standing M-plane GaN substrate with a length of 26 mm, a width of 17 mm, and a thickness of 470 ⁇ m and having a rectangular principal surface with a long side parallel to an a-axis and a short side parallel to a c-axis was fabricated by a method substantially the same as that used for the tertiary substrate fabricated in 4.1.1. [3] above.
  • the M-plane GaN substrate was annealed by placing in an atmosphere containing nitrogen gas and ammonia at a volumetric ratio of 9:1 at 1000°C for 50 hours.
  • oxides adhered to the surface were removed and, furthermore, both principal surfaces were subjected to lapping and CMP.
  • the size of the substrate after these processings was 26 mm in an a-axis direction, 16 mm in a c-axis direction, and 350 ⁇ m in an m-axis direction.
  • Fig. 27 (a) shows an external view photograph of the test piece.
  • An X-ray topography apparatus (product name: XRT micron) by Rigaku Corporation was used for X-ray topography.
  • MoK ⁇ was used as an X-ray source and an X-ray CCD camera with a pixel size of 5.4 ⁇ m was used as a detector.
  • Fig. 27 (b) is a transmission X-ray topograph of the test piece obtained using (002) diffraction.
  • Fig. 27(d) is a reflection X-ray topograph of the same test piece obtained using (203) diffraction. As shown in the diagram, the reflection topograph exhibited extremely high uniformity over the entire 12 mm ⁇ 12 mm region. Accordingly, it is conceivable that the light and shade observed in the anomalous transmission X-ray topograph reflect distortion or defects existing inside the substrate.
  • a 350 ⁇ m-thick self-standing M-plane GaN substrate with a longitudinal direction parallel to an a-axis was fabricated by a method substantially the same as that used for the tertiary substrate fabricated in 4.1.1. [3] above. Annealing was not performed in Experiment 5-2.
  • Fig. 28 (a) shows an external view photograph of the fabricated substrate.
  • the size of the principal surface was 35 mm (total length) in an a-axis direction and 15 mm in a c-axis direction.
  • Fig. 28(b) is a transmission X-ray topograph of the self-standing M-plane GaN substrate obtained using (002) diffraction.
  • the X-RAY Topographic Imaging System XRT-300 by Rigaku Corporation was used for the measurement.
  • MoK ⁇ was used as an X-ray source and an imaging plate with a pixel size of 50 ⁇ m was used as a detector.
  • the a-axis length on a principal surface of the self-standing M-plane GaN substrate of Experiment 5-2 was measured every 250 ⁇ m on straight lines parallel to the c-axis using the high-resolution X-ray diffractometer described previously. As schematically shown in Fig. 29 , measurements were respectively performed on five straight lines A to E arranged at 5 mm intervals in an a-axis direction.
  • a-axis length on the principal surface of the self-standing M-plane GaN substrate of Experiment 5-2 was measured every 250 ⁇ m on a straight line parallel to the a-axis using the high-resolution X-ray diffractometer described previously. Results thereof are shown in Fig. 35 .
  • a self-standing M-plane GaN substrate having a rectangular principal surface was fabricated using, as a material, a GaN crystal fabricated by a method substantially the same as that used for the tertiary GaN crystal fabricated in 4.1.1. [3] above.
  • the principal surface had a size of 26 mm in an a-axis direction and 15 mm in a c-axis direction.
  • an a-axis length and a c-axis length were measured every 250 ⁇ m along a c-axis direction using the high-resolution X-ray diffractometer described previously.
  • the a-axis length had a variation width of 5.2 ⁇ 10 -5 A with the exception of end portions.
  • the c-axis length had a variation width of 1.9 ⁇ 10 -5 ⁇ as shown in Fig. 37 .
  • a self-standing M-plane GaN substrate having a rectangular principal surface was fabricated by a method substantially the same as that used for the tertiary substrate fabricated in 4.1.1. [3] above.
  • the principal surface had a size of 16 mm in an a-axis direction and 10 mm in a c-axis direction.
  • a region excluding portions at a distance of 2 mm or less from a substrate end surface, of the principal surface, was assumed to be an effective region, and the total number of dislocations existing in the effective region was measured. Then, the total number of dislocations was divided by an area of the effective region to obtain a dislocation density of 1.3 ⁇ 10 4 cm -2 .
  • a stacking fault density obtained by dividing a total length of stacking faults existing in the effective region by the area of the effective region was 0.05 cm -1 .
  • a GaN crystal was further grown by an ammonothermal method using the self-standing GaN substrate as a seed.
  • a self-standing GaN (30-3-1) substrate with a rectangular principal surface was fabricated.
  • the principal surface had a size of 21 to 29 mm in an a-axis direction and a size of 10 to 18 mm in a direction perpendicular to the a-axis.
  • the dislocation density of the substrate with a lowest dislocation density was 9. 0 ⁇ 10 2 cm -2 and the dislocation density of the substrate with a highest dislocation density was 6.3 ⁇ 10 4 cm -2 .
  • a GaN thin film was grown on the principal surface by an MOCVD method and a surface of the thin film was observed by an optical microscope to investigate lengths of stacking faults existing in the effective region. Subsequently, the total value of the lengths of the stacking faults was divided by an area of the effective region to obtain a stacking fault density. As a result, the stacking fault density of the substrate with a lowest stacking fault density was 0 cm -1 and the stacking fault density of the substrate with a highest stacking fault density was 1 cm -1 .
  • the a-axis length had a variation width of 5.5 ⁇ 10 -5 ⁇ .
  • the c-axis length had a variation width of 1. 9 ⁇ 10 -4 ⁇ with the exception of end portions.
  • a GaN crystal was further grown by an ammonothermal method using the self-standing GaN substrate as a seed.
  • a self-standing GaN (20-21) substrate with a rectangular principal surface was fabricated.
  • the principal surface had a size of 23 to 26 mm in an a-axis direction and a size of 9 to 12 mm in a direction perpendicular to the a-axis.
  • a region excluding portions at a distance of 2 mm or less from a substrate end surface, of the principal surface was assumed to be an effective region and the total number of dislocations existing in the effective region was measured. Then, the total number of dislocations was divided by an area of the effective region to obtain a dislocation density.
  • the dislocation density of the substrate with a lowest dislocation density was 4.0 ⁇ 10 4 cm -2 and the dislocation density of the substrate with a highest dislocation density was 1.6 ⁇ 10 5 cm -2 .
  • a GaN thin film was grown on the principal surface by an MOCVD method and a surface of the thin film was observed by an optical microscope to investigate lengths of stacking faults existing in the effective region. Subsequently, the total value of the lengths of the stacking faults was divided by an area of the effective region to obtain a stacking fault density. As a result, the stacking fault density of the substrate with a lowest stacking fault density was 0 cm -1 and the stacking fault density of the substrate with a highest stacking fault density was 1 cm -1 .
  • the M-plane GaN substrate of Experiment 7 has a large crystal disturbance at an end portion whose position in a c-axis direction is less than -2 mm.
  • the a-axis length had a variation width of 5.9 ⁇ 10 -5 ⁇ and the c-axis length had a variation width of 1.7 ⁇ 10 -4 ⁇ .
  • a seed substrate with a small angle between the normal of the principal surface and an M-plane may be advantageously used.

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US20180072570A1 (en) * 2015-03-30 2018-03-15 Tosoh Corporation Gallium nitride-based sintered compact and method for manufacturing same
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JP6760285B2 (ja) * 2015-07-14 2020-09-23 三菱ケミカル株式会社 非極性または半極性GaNウエハ
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KR102383392B1 (ko) * 2016-09-30 2022-04-08 한국전자통신연구원 질화물 반도체의 결함 검사 방법
CN106449894B (zh) * 2016-12-08 2017-10-03 西安电子科技大学 基于双异质结的Ga2O3/GaN/SiC光电探测二极管及其制备方法
JP6266742B1 (ja) * 2016-12-20 2018-01-24 古河機械金属株式会社 Iii族窒化物半導体基板、及び、iii族窒化物半導体基板の製造方法
JP6831276B2 (ja) 2017-03-17 2021-02-17 古河機械金属株式会社 Iii族窒化物半導体基板
JP7112879B2 (ja) 2018-05-15 2022-08-04 株式会社サイオクス 窒化物半導体積層物の製造方法、膜質検査方法および半導体成長装置の検査方法
KR20210041077A (ko) 2018-08-17 2021-04-14 미쯔비시 케미컬 주식회사 n 형 GaN 결정, GaN 웨이퍼, 그리고, GaN 결정, GaN 웨이퍼 및 질화물 반도체 디바이스의 제조 방법

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